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The quantum Ising chain for beginners

Published 19 Sep 2020 in quant-ph and cond-mat.quant-gas | (2009.09208v2)

Abstract: We present here various techniques to work with clean and disordered quantum Ising chains, for the benefit of students and non-experts. Starting from the Jordan-Wigner transformation, which maps spin-1/2 systems into fermionic ones, we review some of the basic approaches to deal with the superconducting correlations that naturally emerge in this context. In particular, we analyse the form of the ground state and excitations of the model, relating them to the symmetry-breaking physics, and illustrate aspects connected to calculating dynamical quantities, thermal averages, correlation functions and entanglement entropy. A few problems provide simple applications of the techniques.

Citations (69)

Summary

  • The paper presents a comprehensive mapping of spin models to fermionic systems through the Jordan-Wigner transformation.
  • It employs the Bogoliubov transformation to solve for ground and excited states, revealing symmetry-breaking and topological effects.
  • The study investigates non-equilibrium dynamics and disorder-induced localization, providing actionable insights for experimental quantum simulators.

An Overview of Techniques for Quantum Ising Chains

The study of quantum many-body systems has long fascinated researchers across the fields of condensed matter physics and quantum information science. One canonical model that serves as a paradigmatic example of non-trivial quantum dynamics is the quantum Ising chain. The paper in discussion offers a comprehensive introduction to the methods and techniques for analyzing both clean and disordered quantum Ising chains, particularly focusing on how these systems can be mapped and studied using fermionic representations.

The paper begins by outlining the theoretical framework for mapping spin-1/2 systems into fermionic systems using the Jordan-Wigner transformation. This transformation is central to simplifying the Hamiltonian of the quantum Ising chain from a spin model to a more tractable problem of free fermions. Such a mapping is particularly convenient in one-dimensional systems where the otherwise complex problem of interacting spins is transformed into a problem involving fermions that are subject to quadratic Hamiltonians, making it amenable to exact diagonalization.

In the context of a clean quantum Ising model, the discussion is extended to include the solution of the model using the Bogoliubov transformation, allowing for analytical access to the ground states and excitations of the system. It highlights the role of symmetry-breaking physics and topological features wherein Majorana modes appear in the ferromagnetic phase, especially with open boundary conditions. The intricate connection to the theory of topological superconductivity is emphasized through the illustration of how zero-energy boundary modes appear, illustrating the profound consequences of symmetry and topology in these systems.

The paper does not limit itself to equilibrium properties. On the contrary, the authors explore the non-equilibrium dynamics of the system using time-dependent Bogoliubov-de Gennes (BdG) equations. These equations serve as a powerful toolkit to explore how initially prepared ground states evolve when subject to time-dependent perturbations or quenches in the Hamiltonian. Such studies are relevant in recent experiments involving quantum simulators, like trapped ions and Rydberg atoms.

Additionally, a noteworthy exploration is made into the implications of randomness and disorder. The authors examine how the introduction of disorder in the couplings of the Ising chain leads to phenomena such as Anderson localization, highlighting the differences in behavior from the clean case. This is critical as it touches upon areas like many-body localization, which have been of significant recent interest.

Further sections of the paper provide practical guidance on calculating spin-spin correlation functions and the entanglement entropy—a measure quantifying quantum correlations within the system. These properties are crucial for characterizing quantum phase transitions and different scaling behaviors at critical points.

While the mathematical intricacies and advanced methods are the backbone of this paper, its implications stretch far in both theoretical and experimental landscapes. The tractable models discussed serve as testing grounds for concepts that apply to real-world materials, having similar quantum phase transitions and localized behaviors.

In conclusion, the methodologies elaborated on in this paper, including the Jordan-Wigner transformation, Bogoliubov and Nambu formalisms, and the handling of disorder effects, provide a robust framework for understanding and simulating complex quantum Ising systems. The dialog between theoretical models and their applicability to experimental systems is especially beneficial, setting the stage for future exploration into quantum many-body dynamics and potential quantum technologies.

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